πd3/16
πd3/32
πd4/32
πd4/64
C. πd4/32
Change
Does not change
Changes periodically
None of these
One point
Two points
Plane
Perpendicular planes
W sinθ
W cosθ
W tanθ
W cotθ
h/kG
h2/kG
kG2/h
h × kG
1 + m
1 - m
1 / m
m
[√(4p² - q²)]/6
(4p² - q²)/6
(p² - q²)/4
(p² + q²)/4
Angle of friction
Angle of repose
Angle of banking
None of these
First
Second
Third
None of these
Magnitude
Direction
Point of application
All of the above
Weight
Velocity
Acceleration
Force
A force acting in the opposite direction to the motion of the body is called force of friction
The ratio of the limiting friction to the normal reaction is called coefficient of friction
A machine whose efficiency is 100% is known as an ideal machine
The velocity ratio of a machine is the ratio of load lifted to the effort applied
Lie on the same line
Meet at one point
Meet on the same plane
None of these
kilogram
Newton
Watt
Dyne
mr2/3
2mr2/3
2mr2/5
3mr2/5
W sinθ
W cosθ
W tanθ
None of these
Same
Half
Double
None of these
D + d
D - d
D × d
D / d
The three forces must be equal
The three forces must be at 120° to each other
The three forces must be in equilibrium
If the three forces acting at a point are in equilibrium, then each force is proportional to the sine of the angle between the other two
Concurrence of the medians
Intersection of its altitudes
Intersection of bisector of angles
Intersection of diagonals
The two bodies will momentarily come to rest after collision
The two bodies tend to compress and deform at the surface of contact
The two bodies begin to regain their original shape
All of the above
ω
ωr
ω2r
ω/r
If any number of forces acting at a point can be represented by the sides of a polygon taken in order, then the forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon, then the forces are in equilibrium
If a polygon representing forces acting at a point is closed then forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon taken in order, then the forces are in equilibrium
Inward
Outward
Towards front
Towards back
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
2P sinθ/2
2P cosθ/2
2P tanθ/2
2P cotθ/2
Coplanar concurrent forces
Coplanar non-concurrent forces
Like parallel forces
Unlike parallel forces
[m₁ m₂/2(m₁ + m₂)] (u₁ - u₂)²
[2(m₁ + m₂)/m₁ m₂] (u₁ - u₂)²
[m₁ m₂/2(m₁ + m₂)] (u₁² - u₂²)
[2(m₁ + m₂)/m₁ m₂] (u₁² - u₂²)
Dyne
Watt
kg-m
Joule
The point of C.G.
The point of metacenter
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
Point of suspension
5
10
20
40